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Geant4/examples/extended/hadronic/Hadr02/include/CRMC_FTFP_BERT.hh

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Differences between /examples/extended/hadronic/Hadr02/include/CRMC_FTFP_BERT.hh (Version 11.3.0) and /examples/extended/hadronic/Hadr02/include/CRMC_FTFP_BERT.hh (Version 11.1.2)


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 26 /// \file hadronic/Hadr02/include/CRMC_FTFP_BE     26 /// \file hadronic/Hadr02/include/CRMC_FTFP_BERT.hh
 27 /// \brief Definition of the CRMC_FTFP_BERT cl     27 /// \brief Definition of the CRMC_FTFP_BERT class
 28 //                                                 28 //
 29 //                                                 29 //
 30 //--------------------------------------------     30 //---------------------------------------------------------------------------
 31 //                                                 31 //
 32 // ClassName: CRMC_FTFP_BERT                   <<  32 // ClassName: CRMC_FTFP_BERT  
 33 //                                                 33 //
 34 // Author:    2018 Alberto Ribon                   34 // Author:    2018 Alberto Ribon
 35 //                                                 35 //
 36 // This is a variant of the FTFP_BERT physics  <<  36 // This is a variant of the FTFP_BERT physics list, whereby CRMC is used 
 37 // for modeling final-state pion- , kaon- , pr <<  37 // for modeling final-state pion- , kaon- , proton- , neutron- and 
 38 // ion-nuclear inelastic interactions at very      38 // ion-nuclear inelastic interactions at very high energies (above a
 39 // threshold defined in HadronPhysicsCRMC_FTFP     39 // threshold defined in HadronPhysicsCRMC_FTFP_BERT and IonCRMCPhysics).
 40 // For the remaining inelastic interactions (i     40 // For the remaining inelastic interactions (i.e. hyperon- , antihyperon- ,
 41 // antinucleon- and light anti-ion-nuclear int     41 // antinucleon- and light anti-ion-nuclear interactions, as well as
 42 // for all elastic final-state interactions, a     42 // for all elastic final-state interactions, and for all elastic and
 43 // inelastic hadronic cross sections), the usu     43 // inelastic hadronic cross sections), the usual Geant4 approach, as in
 44 // FTFP_BERT is used.                              44 // FTFP_BERT is used.
 45 //                                                 45 //
 46 // Modified:                                       46 // Modified:
 47 // -  18-May-2021 Alberto Ribon : Migrated to      47 // -  18-May-2021 Alberto Ribon : Migrated to non-templated physics list.
 48 //                                                 48 //
 49 //--------------------------------------------     49 //----------------------------------------------------------------------------
 50 //                                                 50 //
 51 #ifndef CRMC_FTFP_BERT_h                           51 #ifndef CRMC_FTFP_BERT_h
 52 #define CRMC_FTFP_BERT_h 1                         52 #define CRMC_FTFP_BERT_h 1
 53                                                    53 
 54 #include "G4VModularPhysicsList.hh"            << 
 55 #include "globals.hh"                              54 #include "globals.hh"
                                                   >>  55 #include "G4VModularPhysicsList.hh"
                                                   >>  56 
 56                                                    57 
 57 class CRMC_FTFP_BERT : public G4VModularPhysic <<  58 class CRMC_FTFP_BERT : public G4VModularPhysicsList {
 58 {                                              << 
 59   public:                                          59   public:
 60     CRMC_FTFP_BERT(G4int ver = 1);             <<  60     CRMC_FTFP_BERT( G4int ver = 1 );
 61     virtual ~CRMC_FTFP_BERT() = default;           61     virtual ~CRMC_FTFP_BERT() = default;
 62                                                    62 
 63     CRMC_FTFP_BERT(const CRMC_FTFP_BERT&) = de <<  63     CRMC_FTFP_BERT( const CRMC_FTFP_BERT & ) = delete;
 64     CRMC_FTFP_BERT& operator=(const CRMC_FTFP_ <<  64     CRMC_FTFP_BERT & operator=( const CRMC_FTFP_BERT & ) = delete;  
 65 };                                                 65 };
 66                                                    66 
 67 #endif                                             67 #endif
 68                                                    68